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Phragmén–Lindelöf principle

In complex analysis, the Phragmén–Lindelöf principle (or method), first formulated by Lars Edvard Phragmén (1863–1937) and Ernst Leonard Lindelöf (1870–1946) in 1908, is a technique which employs an auxiliary, parameterized function to prove the boundedness of a holomorphic function (i.e, ) on an unbounded domain when an additional (usually mild) condition constraining the growth of on is given. It is a generalization of the maximum modulus principle, which is only applicable to bounded domains.

Background edit

In the theory of complex functions, it is known that the modulus (absolute value) of a holomorphic (complex differentiable) function in the interior of a bounded region is bounded by its modulus on the boundary of the region. More precisely, if a non-constant function   is holomorphic in a bounded region[1]   and continuous on its closure  , then   for all  . This is known as the maximum modulus principle. (In fact, since   is compact and   is continuous, there actually exists some   such that  .) The maximum modulus principle is generally used to conclude that a holomorphic function is bounded in a region after showing that it is bounded on its boundary.

However, the maximum modulus principle cannot be applied to an unbounded region of the complex plane. As a concrete example, let us examine the behavior of the holomorphic function   in the unbounded strip

 .

Although  , so that   is bounded on boundary  ,   grows rapidly without bound when   along the positive real axis. The difficulty here stems from the extremely fast growth of   along the positive real axis. If the growth rate of   is guaranteed to not be "too fast," as specified by an appropriate growth condition, the Phragmén–Lindelöf principle can be applied to show that boundedness of   on the region's boundary implies that   is in fact bounded in the whole region, effectively extending the maximum modulus principle to unbounded regions.

Outline of the technique edit

Suppose we are given a holomorphic function   and an unbounded region  , and we want to show that   on  . In a typical Phragmén–Lindelöf argument, we introduce a certain multiplicative factor   satisfying   to "subdue" the growth of  . In particular,   is chosen such that (i):   is holomorphic for all   and   on the boundary   of an appropriate bounded subregion  ; and (ii): the asymptotic behavior of   allows us to establish that   for   (i.e., the unbounded part of   outside the closure of the bounded subregion). This allows us to apply the maximum modulus principle to first conclude that   on   and then extend the conclusion to all  . Finally, we let   so that   for every   in order to conclude that   on  .

In the literature of complex analysis, there are many examples of the Phragmén–Lindelöf principle applied to unbounded regions of differing types, and also a version of this principle may be applied in a similar fashion to subharmonic and superharmonic functions.

Example of application edit

To continue the example above, we can impose a growth condition on a holomorphic function   that prevents it from "blowing up" and allows the Phragmén–Lindelöf principle to be applied. To this end, we now include the condition that

 

for some real constants   and  , for all  . It can then be shown that   for all   implies that   in fact holds for all  . Thus, we have the following proposition:

Proposition. Let

 

Let   be holomorphic on   and continuous on  , and suppose there exist real constants   such that

 

for all   and   for all  . Then   for all  .

Note that this conclusion fails when  , precisely as the motivating counterexample in the previous section demonstrates. The proof of this statement employs a typical Phragmén–Lindelöf argument:[2]

Proof: (Sketch) We fix   and define for each   the auxiliary function   by  . Moreover, for a given  , we define   to be the open rectangle in the complex plane enclosed within the vertices  . Now, fix   and consider the function  . Because one can show that   for all  , it follows that   for  . Moreover, one can show for   that   uniformly as  . This allows us to find an   such that   whenever   and  . Now consider the bounded rectangular region  . We have established that   for all  . Hence, the maximum modulus principle implies that   for all  . Since   also holds whenever   and  , we have in fact shown that   holds for all  . Finally, because   as  , we conclude that   for all  . Q.E.D.

Phragmén–Lindelöf principle for a sector in the complex plane edit

A particularly useful statement proved using the Phragmén–Lindelöf principle bounds holomorphic functions on a sector of the complex plane if it is bounded on its boundary. This statement can be used to give a complex analytic proof of the Hardy's uncertainty principle, which states that a function and its Fourier transform cannot both decay faster than exponentially.[3]

Proposition. Let   be a function that is holomorphic in a sector

 

of central angle  , and continuous on its boundary. If

 

 

 

 

 

(1)

for  , and

 

 

 

 

 

(2)

for all  , where   and  , then   holds also for all  .

Remarks edit

The condition (2) can be relaxed to

 

 

 

 

 

(3)

with the same conclusion.

Special cases edit

In practice the point 0 is often transformed into the point ∞ of the Riemann sphere. This gives a version of the principle that applies to strips, for example bounded by two lines of constant real part in the complex plane. This special case is sometimes known as Lindelöf's theorem.

Carlson's theorem is an application of the principle to functions bounded on the imaginary axis.

See also edit

References edit

  1. ^ The term region is not uniformly employed in the literature; here, a region is taken to mean a nonempty connected open subset of the complex plane.
  2. ^ Rudin, Walter (1987). Real and Complex Analysis. New York: McGraw-Hill. pp. 257–259. ISBN 0070542341.
  3. ^ Tao, Terence (2009-02-18). "Hardy's Uncertainty Principle". Updates on my research and expository papers, discussion of open problems, and other maths-related topics. By Terence Tao.
  • Phragmén, Lars Edvard; Lindelöf, Ernst (1908). "Sur une extension d'un principe classique de l'analyse et sur quelques propriétés des fonctions monogènes dans le voisinage d'un point singulier". Acta Math. 31 (1): 381–406. doi:10.1007/BF02415450. ISSN 0001-5962.
  • Riesz, Marcel (1920). "Sur le principe de Phragmén-Lindelöf". Proceedings of the Cambridge Philosophical Society. 20. (Corr. "Sur le principe de Phragmén-Lindelöf". 21. 1921. {{cite journal}}: Cite journal requires |journal= (help))
  • Titchmarsh, Edward Charles (1976). The Theory of Functions (Second ed.). Oxford University Press. ISBN 0-19-853349-7. (See chapter 5)
  • E.D. Solomentsev (2001) [1994], "Phragmén–Lindelöf theorem", Encyclopedia of Mathematics, EMS Press
  • Stein, Elias M. and Shakarchi, Rami (2003). Complex analysis. Princeton Lectures in Analysis, II. Princeton, NJ: Princeton University Press. ISBN 0-691-11385-8.{{cite book}}: CS1 maint: multiple names: authors list (link)

phragmén, lindelöf, principle, complex, analysis, method, first, formulated, lars, edvard, phragmén, 1863, 1937, ernst, leonard, lindelöf, 1870, 1946, 1908, technique, which, employs, auxiliary, parameterized, function, prove, boundedness, holomorphic, functio. In complex analysis the Phragmen Lindelof principle or method first formulated by Lars Edvard Phragmen 1863 1937 and Ernst Leonard Lindelof 1870 1946 in 1908 is a technique which employs an auxiliary parameterized function to prove the boundedness of a holomorphic function f displaystyle f i e f z lt M z W displaystyle f z lt M z in Omega on an unbounded domain W displaystyle Omega when an additional usually mild condition constraining the growth of f displaystyle f on W displaystyle Omega is given It is a generalization of the maximum modulus principle which is only applicable to bounded domains Contents 1 Background 2 Outline of the technique 3 Example of application 4 Phragmen Lindelof principle for a sector in the complex plane 4 1 Remarks 5 Special cases 6 See also 7 ReferencesBackground editIn the theory of complex functions it is known that the modulus absolute value of a holomorphic complex differentiable function in the interior of a bounded region is bounded by its modulus on the boundary of the region More precisely if a non constant function f C C displaystyle f mathbb C to mathbb C nbsp is holomorphic in a bounded region 1 W displaystyle Omega nbsp and continuous on its closure W W W displaystyle overline Omega Omega cup partial Omega nbsp then f z0 lt supz W f z textstyle f z 0 lt sup z in partial Omega f z nbsp for all z0 W displaystyle z 0 in Omega nbsp This is known as the maximum modulus principle In fact since W displaystyle overline Omega nbsp is compact and f displaystyle f nbsp is continuous there actually exists some w0 W displaystyle w 0 in partial Omega nbsp such that f w0 supz W f z textstyle f w 0 sup z in Omega f z nbsp The maximum modulus principle is generally used to conclude that a holomorphic function is bounded in a region after showing that it is bounded on its boundary However the maximum modulus principle cannot be applied to an unbounded region of the complex plane As a concrete example let us examine the behavior of the holomorphic function f z exp exp z displaystyle f z exp exp z nbsp in the unbounded strip S z ℑ z p2 p2 displaystyle S left z Im z in left frac pi 2 frac pi 2 right right nbsp Although f x pi 2 1 displaystyle f x pm pi i 2 1 nbsp so that f displaystyle f nbsp is bounded on boundary S displaystyle partial S nbsp f displaystyle f nbsp grows rapidly without bound when z displaystyle z to infty nbsp along the positive real axis The difficulty here stems from the extremely fast growth of f displaystyle f nbsp along the positive real axis If the growth rate of f displaystyle f nbsp is guaranteed to not be too fast as specified by an appropriate growth condition the Phragmen Lindelof principle can be applied to show that boundedness of f displaystyle f nbsp on the region s boundary implies that f displaystyle f nbsp is in fact bounded in the whole region effectively extending the maximum modulus principle to unbounded regions Outline of the technique editSuppose we are given a holomorphic function f displaystyle f nbsp and an unbounded region S displaystyle S nbsp and we want to show that f M displaystyle f leq M nbsp on S displaystyle S nbsp In a typical Phragmen Lindelof argument we introduce a certain multiplicative factor hϵ displaystyle h epsilon nbsp satisfying limϵ 0hϵ 1 textstyle lim epsilon to 0 h epsilon 1 nbsp to subdue the growth of f displaystyle f nbsp In particular hϵ displaystyle h epsilon nbsp is chosen such that i fhϵ displaystyle fh epsilon nbsp is holomorphic for all ϵ gt 0 displaystyle epsilon gt 0 nbsp and fhϵ M displaystyle fh epsilon leq M nbsp on the boundary Sbdd displaystyle partial S mathrm bdd nbsp of an appropriate bounded subregion Sbdd S displaystyle S mathrm bdd subset S nbsp and ii the asymptotic behavior of fhϵ displaystyle fh epsilon nbsp allows us to establish that fhϵ M displaystyle fh epsilon leq M nbsp for z S Sbdd displaystyle z in S setminus overline S mathrm bdd nbsp i e the unbounded part of S displaystyle S nbsp outside the closure of the bounded subregion This allows us to apply the maximum modulus principle to first conclude that fhϵ M displaystyle fh epsilon leq M nbsp on Sbdd displaystyle overline S mathrm bdd nbsp and then extend the conclusion to all z S displaystyle z in S nbsp Finally we let ϵ 0 displaystyle epsilon to 0 nbsp so that f z hϵ z f z displaystyle f z h epsilon z to f z nbsp for every z S displaystyle z in S nbsp in order to conclude that f M displaystyle f leq M nbsp on S displaystyle S nbsp In the literature of complex analysis there are many examples of the Phragmen Lindelof principle applied to unbounded regions of differing types and also a version of this principle may be applied in a similar fashion to subharmonic and superharmonic functions Example of application editTo continue the example above we can impose a growth condition on a holomorphic function f displaystyle f nbsp that prevents it from blowing up and allows the Phragmen Lindelof principle to be applied To this end we now include the condition that f z lt exp Aexp c ℜ z displaystyle f z lt exp left A exp c cdot left Re z right right nbsp for some real constants c lt 1 displaystyle c lt 1 nbsp and A lt displaystyle A lt infty nbsp for all z S displaystyle z in S nbsp It can then be shown that f z 1 displaystyle f z leq 1 nbsp for all z S displaystyle z in partial S nbsp implies that f z 1 displaystyle f z leq 1 nbsp in fact holds for all z S displaystyle z in S nbsp Thus we have the following proposition Proposition Let S z ℑ z p2 p2 S z ℑ z p2 p2 displaystyle S left z Im z in left frac pi 2 frac pi 2 right right quad overline S left z Im z in left frac pi 2 frac pi 2 right right nbsp Let f displaystyle f nbsp be holomorphic on S displaystyle S nbsp and continuous on S displaystyle overline S nbsp and suppose there exist real constants c lt 1 A lt displaystyle c lt 1 A lt infty nbsp such that f z lt exp Aexp c ℜ z displaystyle f z lt exp bigl A exp c cdot Re z bigr nbsp for all z S displaystyle z in S nbsp and f z 1 displaystyle f z leq 1 nbsp for all z S S S displaystyle z in overline S setminus S partial S nbsp Then f z 1 displaystyle f z leq 1 nbsp for all z S displaystyle z in S nbsp Note that this conclusion fails when c 1 displaystyle c 1 nbsp precisely as the motivating counterexample in the previous section demonstrates The proof of this statement employs a typical Phragmen Lindelof argument 2 Proof Sketch We fix b c 1 displaystyle b in c 1 nbsp and define for each ϵ gt 0 displaystyle epsilon gt 0 nbsp the auxiliary function hϵ displaystyle h epsilon nbsp by hϵ z e ϵ ebz e bz textstyle h epsilon z e epsilon e bz e bz nbsp Moreover for a given a gt 0 displaystyle a gt 0 nbsp we define Sa displaystyle S a nbsp to be the open rectangle in the complex plane enclosed within the vertices a ip 2 a ip 2 displaystyle a pm i pi 2 a pm i pi 2 nbsp Now fix ϵ gt 0 displaystyle epsilon gt 0 nbsp and consider the function fhϵ displaystyle fh epsilon nbsp Because one can show that hϵ z 1 displaystyle h epsilon z leq 1 nbsp for all z S displaystyle z in overline S nbsp it follows that f z hϵ z 1 displaystyle f z h epsilon z leq 1 nbsp for z S displaystyle z in partial S nbsp Moreover one can show for z S displaystyle z in overline S nbsp that f z hϵ z 0 displaystyle f z h epsilon z to 0 nbsp uniformly as ℜ z displaystyle Re z to infty nbsp This allows us to find an x0 displaystyle x 0 nbsp such that f z hϵ z 1 displaystyle f z h epsilon z leq 1 nbsp whenever z S displaystyle z in overline S nbsp and ℜ z x0 displaystyle Re z geq x 0 nbsp Now consider the bounded rectangular region Sx0 displaystyle S x 0 nbsp We have established that f z hϵ z 1 displaystyle f z h epsilon z leq 1 nbsp for all z Sx0 displaystyle z in partial S x 0 nbsp Hence the maximum modulus principle implies that f z hϵ z 1 displaystyle f z h epsilon z leq 1 nbsp for all z Sx0 displaystyle z in overline S x 0 nbsp Since f z hϵ z 1 displaystyle f z h epsilon z leq 1 nbsp also holds whenever z S displaystyle z in S nbsp and ℜ z gt x0 displaystyle Re z gt x 0 nbsp we have in fact shown that f z hϵ z 1 displaystyle f z h epsilon z leq 1 nbsp holds for all z S displaystyle z in S nbsp Finally because fhϵ f displaystyle fh epsilon to f nbsp as ϵ 0 displaystyle epsilon to 0 nbsp we conclude that f z 1 displaystyle f z leq 1 nbsp for all z S displaystyle z in S nbsp Q E D Phragmen Lindelof principle for a sector in the complex plane editA particularly useful statement proved using the Phragmen Lindelof principle bounds holomorphic functions on a sector of the complex plane if it is bounded on its boundary This statement can be used to give a complex analytic proof of the Hardy s uncertainty principle which states that a function and its Fourier transform cannot both decay faster than exponentially 3 Proposition Let F displaystyle F nbsp be a function that is holomorphic in a sector S z a lt arg z lt b displaystyle S left z big alpha lt arg z lt beta right nbsp of central angle b a p l displaystyle beta alpha pi lambda nbsp and continuous on its boundary If F z 1 displaystyle F z leq 1 nbsp 1 for z S displaystyle z in partial S nbsp and F z eC z r displaystyle F z leq e C z rho nbsp 2 for all z S displaystyle z in S nbsp where r 0 l displaystyle rho in 0 lambda nbsp and C gt 0 displaystyle C gt 0 nbsp then F z 1 displaystyle F z leq 1 nbsp holds also for all z S displaystyle z in S nbsp Remarks edit The condition 2 can be relaxed to lim infr supa lt 8 lt blog F rei8 rr 0for some0 r lt l displaystyle liminf r to infty sup alpha lt theta lt beta frac log F re i theta r rho 0 quad text for some quad 0 leq rho lt lambda nbsp 3 with the same conclusion Special cases editIn practice the point 0 is often transformed into the point of the Riemann sphere This gives a version of the principle that applies to strips for example bounded by two lines of constant real part in the complex plane This special case is sometimes known as Lindelof s theorem Carlson s theorem is an application of the principle to functions bounded on the imaginary axis See also editHadamard three lines theoremReferences edit The term region is not uniformly employed in the literature here a region is taken to mean a nonempty connected open subset of the complex plane Rudin Walter 1987 Real and Complex Analysis New York McGraw Hill pp 257 259 ISBN 0070542341 Tao Terence 2009 02 18 Hardy s Uncertainty Principle Updates on my research and expository papers discussion of open problems and other maths related topics By Terence Tao Phragmen Lars Edvard Lindelof Ernst 1908 Sur une extension d un principe classique de l analyse et sur quelques proprietes des fonctions monogenes dans le voisinage d un point singulier Acta Math 31 1 381 406 doi 10 1007 BF02415450 ISSN 0001 5962 Riesz Marcel 1920 Sur le principe de Phragmen Lindelof Proceedings of the Cambridge Philosophical Society 20 Corr Sur le principe de Phragmen Lindelof 21 1921 a href Template Cite journal html title Template Cite journal cite journal a Cite journal requires journal help Titchmarsh Edward Charles 1976 The Theory of Functions Second ed Oxford University Press ISBN 0 19 853349 7 See chapter 5 E D Solomentsev 2001 1994 Phragmen Lindelof theorem Encyclopedia of Mathematics EMS Press Stein Elias M and Shakarchi Rami 2003 Complex analysis Princeton Lectures in Analysis II Princeton NJ Princeton University Press ISBN 0 691 11385 8 a href Template Cite book html title Template Cite book cite book a CS1 maint multiple names authors list link Retrieved from https en wikipedia org w index php title Phragmen Lindelof principle amp oldid 1197714224, wikipedia, wiki, book, books, library,

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